Optical head device and birefringent diffraction grating polarizer and polarizing hologram element used therein

Abstract: An optical head device uses a birefringent diffraction grating polarizer configured in a reflection type. The device includes a polarizing hologram element (216) which reflects the light from a light source (210) to a converging lens system and diffracts the polarized light returning from a recording medium. A total reflection film (203) is formed on a surface of a diffraction grating which is provided periodically by an ion exchange region and a dielectric film on a surface of a crystal plate (200) having optically anisotropic characteristics. A polarizing beam splitter film (218) formed on a surface of the polarizing hologram element has reflectivity and transmissivity having dependency on the polarization of the incident light. In another form, a polarizing hologram element includes a polarizing hologram which has diffractive efficiency having dependency on polarization of incident light and a polarizing beam splitter film (218) which has reflectivity and transmissivity having dependency on the polarization of the incident light. The diffracted light is received by multi-split photodetectors. The arrangements enable to make the optical head device compact, light in weight and low cost.

Description: The present invention relates to an optical head device, and more particularly to a birefringent diffraction grating polarizer, a polarizing hologram element and a optical head device using such polarizer or hologram element. The polarizer, especially, the polarizing beam splitter is an element with which a predetermined polarized light beam is obtained by causing the light propagation directions changed in the polarized beams orthogonal to each other. Conventional examples of the polarizing beam splitters often used include a Glan-Thompson prism or a Rochon prism. In one example, the optical path is separated by utilization of differences in the transmission or reflection due to the polarization at cemented surfaces of crystal compounds having large birefringences. In another example, a dielectric multi-layer film is provided at the cemented surface of a compound prism type beam splitter and, by utilization of differences in the interference in the dielectric multi-layer film due to the polarization, the light is caused to be reflected or transmitted. The drawbacks in such elements are that the size thereof is large, the productivity thereof is low, and the cost thereof is high. Also, the polarizer of a bulk type as above only has polarizing functions so that, when it is used for an optical disk head device, there are difficulties in compositely accommodating other functions such as those for focusing error detection and tracking error detection, and these are obstacles to the scaling down of the optical head device. A recently developed polarizer in which the productivity is high and the composite functions other than the polarization function are accommodated is a birefringent diffraction grating polarizer which is disclosed in JP-A-63-314502. Fig. 1 is a sectional view showing such birefringent diffraction grating polarizer. Where a proton exchange region of benzoic acid is provided on an X-plate or a Y-plate of a lithium niobate substrate 1 which is a birefringent crystal, it is noted that, with respect to a wavelength of, for example, 0.78 µm which is generally used in the optical disk device, the index of refraction for ordinary light which is polarized parallel to the crystal optical axis of the substrate increases by about 0.12 and the index of refraction for ordinary light which is polarized perpendicular to the optical axis decreases by about 0.04. Thus, the grating in which the exchange region 2 with the proton and the non-exchange region with the proton are arranged periodically functions as a diffraction grating. When this grating is configured such that a phase compensation film 3 of an appropriate thickness is formed on the exchange region 2 for mutually canceling the phase difference between the ordinary light passing through the exchange region 2 and the ordinary light passing through the non-exchange region, the grating does not function as a diffraction grating with respect to the ordinary light, whereby such ordinary light is allowed to be transmitted without being diffracted. That is, this grating is seen simply as a transparent plate. Where the phase difference with respect to the extraordinary light is π when the depth of the exchange region 2 is changed while maintaining the mutual phase difference cancellation conditions with respect to the ordinary light and, moreover, the width of the proton exchange region 2 and that of the non-exchange region are the same with each other, the extraordinary light is completely diffracted. The relationship of these phases may be expressed by the following equations: {Δn e · T p + (n d - n out )· T d } · 2π/λ = π {Δn o · T p + (n d - n out ) · T d } · 2π/λ = 0 wherein n d and T d are respectively an index of refraction and a thickness of the phase compensation film 3, T p is a depth of the proton exchange region 2, Δn e and Δn o are amounts of changes in the index of refraction in the extraordinary light and the ordinary light at the proton exchange region 2, and n out is an index of refraction outside the hologram substrate, that is, n out = 1 in an air layer. Also, λ is a wavelength of light. Also, it is possible to realize the polarization function by the arrangement wherein the proton exchange region 2 and the phase compensation film 3 are disposed alternately, the phase difference between the light passing through the proton exchange region 2 and the light passing through the phase compensation film 3 of dielectric is made zero with respect to the extraordinary light, the phase difference therebetween is made π with respect to the ordinary light, and the width of the proton exchange region 2 and that of the phase compensation film 3 are made the same with each other. In this case, the extraordinary light is transmitted without being diffracted and the ordinary light is completely diffracted. The disclosure of examples in which the above birefringent diffraction grating polarizer is used in the optical head device is found in JP-A-3-29137 and JP-A-3-29129 corresponding to EP-A-0.405. 444 which respectively disclose hologram elements. While these hologram elements are configured as shown in a sectional view in Fig. 1, the grating patterns are constituted by a plurality of grating regions having different diffraction directions as shown in Fig. 2 for purposes of detecting focusing error signals and tracking error signals in the optical head. In similarly arranged grating patterns, the grating regions are constituted by divided patterns as shown in Fig. 3. Fig. 4 diagrammatically shows an optical head device for use in a video disk, a write once read many type optical disk and a rewritable type phase-change optical disk as disclosed in JP-A-3-29129. The light emitted from a semiconductor laser 10 is incident on a hologram element 16 as ordinary light, transmitted without being diffracted, passes through a collimating lens 11, a 1/4 wavelength plate 13 and an objective lens 12, and is converged on an optical disk 14. The returning light from the optical disk 14 is incident again on the hologram element 16 after passing through the common path in reverse. The polarizing surface of the returning light is rotated 90 degrees with respect to that of the original polarized light by the 1/4 wavelength plate 13 so that such light is incident on the hologram element 16 as extraordinary light and is completely diffracted, and the +1 order diffracted light 50 and the -1 order diffracted light 51 are received respectively by a first photodetector 30 and a second photodetector 31. Fig. 5 shows in a plane view the first photodetector 30 and the second photodetector 31 with the semiconductor laser disposed between them and shows a state of the diffracted light beams incident respectively on the photodetectors. The diffracted light beams from a region 5(A) and the diffracted light beams from a region 6(B) in the hologram (shown in Fig. 2) converge respectively at a converging point 40 and a converging point 41 shown in Fig. 5. A dividing line 9 on the hologram pattern in Fig. 2 functions as a knife edge and, by a double-knife-edge method, a focusing error signal is detected from these diffracted light beams. A tracking error is detected by a push-pull method based on the difference between the diffracted light beams from the region 7(C) and the diffracted light beams from the region 8(D) which converge respectively at the points 42 and 43 shown in Fig. 5. A recording signal is detected based on the light received from the second photodetector 31 or on the sum of the amounts of light received from both the first photodetector 30 and the second photodetector 31. Also, by arranging to receive higher order diffracted beams, it is possible to have the intensity of the signal further increased. Fig. 6 shows an optical head device for a magneto-optical disk as disclosed in JP-A-3-29137. The light emitted from a semiconductor laser 10 passes through a collimating lens 11, a polarizing beam splitter 18 and an objective lens 12 and then is converged on a magneto-optical disk 15. Following a reverse path, the returning light from the magneto-optical disk 15 is separated to outside an optical axis by the polarizing beam splitter 18, is caused to be converged by a lens 19, whereby the extraordinary light component is diffracted by a hologram element 17, and is received by a first photodetector 32, a second photodetector 33 and a third photodetector 34. The polarizing beam splitter 18 has polarization characteristics which cause the p-polarized light from the semiconductor laser 10 to be partially reflected and residually transmitted and also cause the s-polarized light orthogonal thereto, that is, slight amounts of polarized light occurring by Kerr effect at the reflection on the magneto-optical disk 15, to be completely reflected. The recording signal is detected by a differential detection method from the 0 order diffracted light and the +1 order diffracted light separated by polarization due to the polarizing function of the hologram element 17. Where the detection relies on the difference between the sum of +1 order diffracted light 52 and -1 order diffracted light 54 and the 0 order diffracted light 53, the amounts of light become balanced and the recording signal can be detected with small noise when the direction of the returning light is at an angle of 42 degrees with respect to the crystal optical axis of the hologram element. When the detection relies on the difference between the -1 order diffraction light 54 and the 0 order diffracted light 53, the angle may be set to about 32 degrees. Fig. 7 is a diagram for illustrating a state of the diffracted light beams where they are incident on the photodetectors. Focusing and tracking error signals are detected in the same way as in the case of Fig. 5 by using the +1 order diffracted light 52 which is incident on the first photodetector 32. The above described birefringent diffraction grating polarizer is a light transmission type so that the process of forming a grating layer requires a long time because it is necessary to make the proton exchange region deep and also it is necessary to make the phase compensation film thick. Also, if this element is used in the conventional optical head device described above, it will be difficult to make the device compact. Fig. 8 shows a conventional optical head device for use in a magneto-optical disk drive. Emitted light 82 from a semiconductor laser 81 is converted to collimated light 84 by a collimating lens 83 and, after being transmitted through a beam splitter 85 and totally reflected at a total reflection prism 86 with the light path being bent 90 degrees, is converged on an optical disk surface 88 by a convergent lens 87. The reflected light returning from the optical disk follows the common path in reverse and is reflected at the beam splitter 85. The reflected light changes its polarization direction by 90 degrees at a 1/2 wavelength plate 89, is converted to converging light by a lens 90 and is divided by a polarizing beam splitter 93 into the polarized transmission light 91 and the polarized reflection light 92 the polarization directions of which are orthogonal to each other. The transmission light 91 is incident on a half-split photodetector 94, and a tracking error signal is obtained based on a differential signal from photodetector elements 95 and 96 by a push-pull method. On the other hand, the reflection light 92 forms an astigmatic wave surface due to a cylindrical lens 97, and a focusing error signal is obtained through a quarter-split photodetector 98 using an astigmatic method. That is, when the output voltages of photodetector elements 100, 101, 102 and 103 are assumed to be respectively V (100) , V (101) , V (102) and V (103) , the focusing error signal can be obtained by V (100) + V (101) - V (102) - V (103) . The read-out signal is obtained as a differential signal based on intensity differences between the polarized light beams which are split by the polarization beam splitter and the polarization directions of which are orthogonal with each other. Thus, assuming that the output voltages of the photodetector elements 14 and 15 are respectively V (95) and V (96) , the read-out signal will be V (95) + V (96) - V (100) - V (101) -V (102) - V (103) . For the magneto-optical head device utilizing the polarizing hologram, reference is made to Japanese Patent Application Kokai Publication No. Hei 3-29137 which has already been identified above and which discloses the arrangement as shown in Fig. 6. That arrangement employs the polarizing hologram formed by providing ion exchange on a lithium niobate crystal and this enables to reduce the optical system after the 1/2 wavelength plate 89 in Fig. 8 to three elements, namely, the polarizing hologram, lens and photodetectors. However, the above conventional optical head device is still large in size, and a device in practical use is larger than about 40 x 40 x 30 mm and weighs heavy accordingly. This has been a barrier in enhancing high speed tracking access and scaling down of the optical disk device as a whole. EP-A-0 349 144 discloses a birefringent diffraction grating type polarizer. In a birefringence diffraction grating type polarizer, periodic proton ion-exchanged regions are provided on the principal plane surface of an optically anisotropic crystal substrate to provide an optical diffraction grating, and a dielectric layer (3) is provided on each of the periodic proton ion-exchanged regions. The refractive index of the dielectric layer is proximate or equal to that of the crystal substrate, and the whole surface of the optical diffraction grating is covered by an anti-reflection layer of a single material having a uniform thickness. EP-A-0 349 309 relates to a grating type polarizer. A birefringence diffraction grating type polarizer is composed of an optically anisotropic sheet crystal substrate. The optically anisotropic sheet crystal substrate is provided with periodic ion-exchanged regions on the main plane thereof, thereby providing an optical diffraction grating. The ion-exchanged regions are covered with dielectric layers, respectively, and further diffused in the vicinity of the surface thereof with metal. For this structure, it is avoided that a linearly polarized incident light becomes an elliptically polarized light. JP-A-4 143 935 discloses an optical head structure which comprises a transmission grating having polarization characteristics with a partial reflecting plate on one side, and a high reflecting plate placed on the opposite side of the partial reflecting plate with respect to the grating. An object of the invention is to overcome the problems existing in the prior art and to provide a birefringent diffraction grating polarizer in which it is possible to minimize the time for forming the grating layer and fabricating an optical head device which utilizes such polarizer, thereby enabling to further scale down the device. According to the invention, there is provided a birefringent diffraction grating polarizer comprising: a crystal plate having optically anisotropic characteristics; a plurality of ion exchange regions and dielectric films which constitute a diffraction grating and which are formed periodically on a main surface of the crystal plate; and a total reflection film formed on a surface of the diffraction grating. In the above birefringent diffraction grating polarizer, a polarizing beam splitter layer may be formed on a partial region of the surface opposite to the main surface. According to the invention, there is also provided an optical head device comprising: a light source; a converging lens system for converging light beams emitted from the light source on a recording medium; a quarter-wavelength plate for causing a polarized light beam returning from the recording medium to be orthogonal with respect to a polarized light beam emitted from the light source; a hologram element for reflecting the light from the light source to the converging lens system and for reflectively diffracting the light returning from the recording medium; and a photodetector means for receiving the diffracted light, wherein the hologram element comprises a crystal plate having optically anisotropic characteristics, a plurality of ion exchange regions and dielectric films constituting a diffraction grating and being formed periodically on a main surface of the crystal plate, and a total reflection film formed on a surface of the diffraction grating. The birefringent diffraction grating polarizer according to the invention (Figs. 9 - 14B) is configured as a reflection type. In this configuration, since the light reciprocates between the grating layers, the necessary thicknesses of the proton exchange and the phase compensation film of the grating layer can be reduced to less than half as compared with the thicknesses of those of the conventional light transmission type. As already explained with reference to the prior art, the phase difference between the light that passes through the proton exchange region and the light that passes through the region without the proton exchange may be π in the case of extraordinary light and be 0 in the case of ordinary light for the extraordinary light to be diffracted and the ordinary light to be reflected. The phase relationship in such instance can be expressed by the following equations: (Δn e · 2T p ' + n d · 2T d ') · 2π/λ = π (Δn o · 2T p ' + n d · 2T d ') · 2π/λ = π. From the above, T p ' and T d ' may be obtained as follows: T p ' = λ/{4· (Δn e - Δn o )} T d ' = -Δn o /n d · T p '. When the thickness of the proton exchange region and the thickness of the dielectric phase compensation film are compared with those of the prior art transmission type explained above, their relationship may be expressed by the following equations: T p ' = T p /2 T d ' < T d /2. Where the light is incident obliquely on the grating, the optical path length becomes longer as compared with the case wherein the light is incident thereon perpendicularly, the proton region and the phase compensation film can be made still thinner. The above and other objects, features and advantages of the present invention will be apparent from the following description of preferred embodiments of the invention explained with reference to the accompanying drawings, in which: Fig. 1 is a diagrammatic sectional view of a conventional hologram element; Fig. 2 is a diagram showing a grating pattern in a conventional hologram element; Fig. 3 is a diagram showing another grating pattern in the conventional hologram element; Fig. 4 is a diagram showing arrangements of a conventional optical head device; Fig. 5 is a diagram showing a state of diffracted light beams incident on respective photodetectors in a conventional arrangement; Fig. 6 is a diagram showing arrangements of a conventional optical head device; Fig. 7 is a diagram showing a state of diffracted light beams incident on respective photodetectors in a conventional arrangement; Fig. 8 is a perspective view showing arrangements of a conventional optical head device used in a magneto-optical disk device; Fig. 9 is a diagrammatic sectional view of a birefringent diffractive grating polarizer of an embodiment according to the invention; Fig. 10 is a diagrammatic sectional view of a birefringent diffractive grating polarizer of another embodiment according to the invention; Fig. 11A is a diagram showing arrangements of an optical head device of a first embodiment according to the invention; Fig. 11B is a diagram showing a state of diffracted light beams at various detection points in the optical head device of the first embodiment according to the invention; Fig. 12A is a diagram showing arrangements of an optical head device of a second embodiment according to the invention; Fig. 12B is a diagram showing a state of diffracted light beams at various detection points in the optical head device of the second embodiment according to the invention; Fig. 13A is a diagram showing arrangements of an optical head device of a third embodiment according to the invention; Fig. 13B is a diagram showing a state of diffracted light beams at various detection points in the optical head device of the third embodiment according to the invention; Fig. 14A is a diagram showing arrangements of an optical head device of a fourth embodiment according to the invention; and Fig. 14B is a diagram showing a state of diffracted light beams at various detection points in the optical head device of the fourth embodiment according to the invention. Now, preferred embodiments of the invention are explained with reference to the accompanying drawings. Fig. 9 shows in sectional view a birefringent diffraction grating polarizer of an embodiment according to the invention. The dielectric film used as a phase compensation film 202 has a refractive index of 2.2 which is approximately the same as that of a lithium niobate substrate 200. For the light having a wavelength of 0.78 µm, whereas the conventionally configured transmission type requires the phase compensation film to be about 800 nm thick and the proton exchange layer to be about 2.4 µm deep, it is sufficient for the polarizer of the reflection type according to the invention to function if the phase compensation film 202 is about 200 nm thick and the proton exchange region 201 is about 1.2 µm deep. The dielectric film may be formed of Nb 2 O 5 TiO 2 or Ta 2 O 5 . As the total reflection film 203, a metal film or a dielectric multilayer reflection film may be used. Fig. 10 shows in sectional view a birefringent diffraction grating polarizer of another embodiment according to the invention. This embodiment is similar to the embodiment shown in Fig. 9 but is different in that the proton exchange regions 201 and the dielectric phase compensation films 202 are alternately arranged. Fig. 11A shows in a schematically exploded view the optical head device of the first embodiment according to the invention, that is, the optical head device for use in a video disk, a write once read many type optical disk and a rewritable type phase-change optical disk. The hologram element 216 is configured such that the back surface thereof constitutes the birefringent diffraction grating polarizer of a reflection type as explained above, and the grating pattern therein takes the same pattern as in the prior art for the focusing and tracking error signal detection as shown in Figs. 2 and 3. The light from the semi-conductor laser 210 of the light source is incident on the hologram element 216 where the light is in such polarization state that it is reflected without being diffracted at the grating layer therein. The reflected beams are collimated by a collimating lens 211 and are converged on an optical disk 214 after passing through a 1/4 wavelength plate 213 and an objective lens 212. The beams reflected at the optical disk 214 return through the common path and are again incident on the hologram element 216. At this time, the polarization direction of the reflected light is rotated 90 degrees from that of the original light after passing forwardly and rearwardly through the 1/4 wavelength plate 213, so that the light is diffracted at the hologram element 216 and the diffracted beams are received by a first photodetector 230 and a second photodetector 231, respectively. Fig. 11B shows the state of the diffracted beams at various detection points. The focusing and tracking error signals and the recording signals are detected in the same way as in the prior art explained above. Fig. 12A shows in a schematically exploded view an arrangement of the second embodiment according to the invention. In this embodiment, the semiconductor laser 210 and the photodetectors 230 and 231 in the first embodiment are unitarily accommodated in a module 220. Fig. 12B shows such module 220. The beams emitted from the semiconductor laser chip 221 are reflected at the mirror 222 and proceed to the hologram element 216. Also, the beams which return from the hologram element 216 are received by a group of photodetector elements 223, and the focusing and tracking error signals and the recording signals are detected in the same way as already explained. Fig. 13A shows in a schematically exploded view an optical head device of the third embodiment according to the invention, which is for use in the magneto-optical disk. In the hologram element 216, the reflection grating layer 217 is formed at a back surface thereof and a polarizing beam splitter layer 218 is formed at a partial region of a front surface thereof. The reflection grating layer 217 is configured as the reflection type birefringent diffraction grating polarizer as already described, and the grating pattern takes the pattern as in the prior art shown in Fig. 2 or Fig. 3 for detecting focusing and tracking error signals. The polarizing beam splitter layer 218 at the front surface has polarization characteristics which allow most of predetermined polarized beams to be transmitted and cause the polarized beams orthogonal to such predetermined beams to be transmitted and reflected at a predetermined intensity ratio. This can be realized by forming a dielectric multi-layer film at the front surface or by cementing to the front surface a polarizing beam splitting substrate having the above characteristics. The light from the semiconductor laser 210 of the light source is incident on the polarizing beam splitter layer 218 on the hologram element 216 with the above-mentioned polarization state in which the polarized light beams are partly reflected. The reflected beams are collimated by a collimating lens 211 and are converged on a magneto-optical disk 215 after passing through an objective lens 212. The beams reflected at the magneto-optical disk 215 return through the common path in reverse and are incident again on the hologram element 216. The polarizing beam splitter layer 218 has polarization characteristics which allow such beams out of the returning beams as having the original polarization state to be partly transmitted, and cause the beams polarized orthogonal thereto, that is, slight amounts of polarized light occurring by Kerr effect at the reflection on the magneto-optical disk 215, to be mostly transmitted. The light having been transmitted through the polarizing beam splitter layer 218 is diffracted and reflected by the reflecting grating layer 217 at the back surface and the diffracted and the reflected light are received by the photodetector 232. Fig. 13B shows a state of the diffracted light at the photodetector 232. The focusing and tracking error signals are detected from the +1 order diffracted light in the same way as explained with reference to the prior art. Also, as explained for the prior art, by setting an appropriate angle for the polarization direction of the above returning light with respect to the crystal optical axis of the hologram element 216, the recording signal can be detected from a difference between 0 order diffracted light and -1 order diffracted light, or between 0 order diffracted light and ± 1 order diffracted light. Also, if it is arranged that higher order diffracted light be received, it is possible to increase the intensity of the recording signal. Fig. 14A shows a schematically exploded view of an optical head device of the fourth embodiment according to the invention. The semiconductor laser and the photodetector in the above third embodiment are unitarily accommodated in a module 240. Fig. 14B diagrammatically shows the module 240. The light from the semiconductor chip 241 is reflected at the mirror 242 and advances to the hologram element 216. Also, the returning light from the hologram element is incident on a group of photodetector elements 243 and, as already described, the focusing and tracking signals and the recording signals are detected. Since the birefringent diffraction grating polarizer according to the invention is configured in a reflection type, it is possible to reduce the fabrication time and to lower the cost of elements. Also, the optical device can be made compact since the optical head device according to the invention employs a reflection type birefringent diffraction grating polarizer and the optical head device can be made still more compact since the light source and the photodetectors are unitarily arranged in a module form.

Claims: A birefringent diffraction grating polarizer comprising: a crystal plate (200) having optically anisotropic characteristics: a plurality of ion exchange regions (201) and dielectric films (202) which constitute a diffraction grating and which are formed periodically on a main surface of said crystal plate; characterized by a total reflection film (203) formed on a surface of said diffraction grating. A birefringent diffraction grating polarizer according to claim 1, further comprising a polarizing beam splitter layer (218) on a partial region of a surface opposite to said main surface of said crystal plate (200). A polarizer according to claim 1 or 2, in which said dielectric films (202) are arranged on said plurality of ion exchange regions (201). A polarizer according to claim 1 or 2, in which said ion exchange regions (201) and said dielectric films (202) are alternately arranged along the main surface of said crystal plate. A polarizer according to any one of claims 1 to 4, in which said total reflection film (203) is a metal film. An optical head device comprising: a light source (210:221); a converging lens system (211,212) for converging light beams emitted from said light source on a recording medium (214); a quarter-wavelength plate (213) for causing polarized light returning from said recording medium to be orthogonal with respect to polarized light emitted from said light source; a hologram element (216) for reflecting the light from said light source to said converging lens system and for reflectively diffracting the light returning from said recording medium; and a photodetector means (230,231;223) for receiving said diffracted light, wherein said hologram element comprises a crystal plate (200) having optically anisotropic characteristics, a plurality of ion exchange regions (201) and dielectric films (202) constituting a diffraction grating and being formed periodically on a main surface of said crystal plate, and a total reflection film (203) formed on a surface of said diffraction grating. An optical bead device according to claim 6, in which said light source (221) and said photodetector means (223) are accommodated in an integrated module (230). An optical head device according to claim 6 or 7, in which said converging lens system includes a collimating lens (211) and an objective lens (212) with said quarter-wavelength plate (213) being arranged therebetween. An optical head device comprising: a light source (210;241): a converging lens system (211,212) for converging light beams emitted from said light source on a recording medium (214): a hologram element (216) for reflecting the light from said light source to said converging lens system and for reflectively diffracting the light returning from said recording medium; and a photodetector means (232:243) for receiving said diffracted light, wherein said hologram element comprises a crystal plate (200) having optically anisotropic characteristics, a plurality of ion exchange regions (201) and dielectric films (202) constituting a diffraction grating and being formed periodically on a main surface of said crystal plate, a total reflection film (203) formed on a surface of said diffraction grating, and a polarizing beam splitter layer (218) formed on a partial region of a surface opposite to said main surface of said crystal plate. An optical head device according to claim 9, in which said light source (241) and said photodetector means (243) are accommodated in an integrated module (240). An optical head device according to claim 9 or 10, in which said converging lens system includes a collimating lens (211) and an objective lens (212).

Inventors: OBA AKITOMO, ONO YUZO, OBA, AKITOMO, ONO, YUZO, OBA, AKITOMO, C/O NEC CORPORATION, ONO, YUZO, C/O NEC CORPORATION
Applicants: NIPPON ELECTRIC CO, NEC CORPORATION
Application year: 1994
Main classification: G11B11
IPC codes: G02B5, G11B11, G11B7, G02B27